Questions tagged [fourier-analysis]

Fourier analysis, also known as spectral analysis, encompasses all sorts of Fourier expansions, including Fourier series, Fourier transform and the discrete Fourier transform (and relatives). The non-commutative analog is (representation-theory).

Fourier analysis is the study of how general functions can be decomposed into trigonometric or exponential functions with definite frequencies. There are two types of Fourier expansions:

  • Fourier series: If a (reasonably well-behaved) function is periodic, then it can be written as a discrete sum of trigonometric or exponential functions with specific frequencies.
  • Fourier transform: A general function that isn’t necessarily periodic (but that is still reasonably well-behaved) can be written as a continuous integral of trigonometric or exponential functions with a continuum of possible frequencies.

The reason why Fourier analysis is so important is that many (although certainly not all) of the differential equations that govern physical systems are linear, which implies that the sum of two solutions is again a solution. Therefore, since Fourier analysis tells us that any function can be written in terms of sinusoidal functions, we can limit our attention to these functions when solving the differential equations. And then we can build up any other function from these special ones. This is a very helpful strategy, because it is invariably easier to deal with sinusoidal functions than general ones.

Fourier series

Consider a function $f(x)$ that is periodic on the interval $0 ≤ x ≤ L$, then Fourier’s theorem states that $f(x)$ can be written as $$f(x)={a_0}+\sum_{n=1}^{\infty}\left[a_n \cos\left(\frac{2n\pi x}{L}\right)+b_n \sin \left(\frac{2n\pi x}{L}\right)\right]$$ where the constant coefficients $a_n$ and $b_n$ are called the Fourier coefficients of $f$ and is given by $$a_0=\frac{1}{L}\int_0^L f(x)\mathrm{d}x$$ $$a_n=\frac{2}{L}\int_0^L f(x)\cos\left(\frac{2\pi nx }{L}\right)\mathrm{d}x$$ $$b_n=\frac{2}{L}\int_0^L f(x)\sin\left(\frac{2\pi nx }{L}\right)\mathrm{d}x$$

Reference:

http://www.people.fas.harvard.edu/~djmorin/waves/Fourier.pdf

https://en.wikipedia.org/wiki/Fourier_analysis

http://mathworld.wolfram.com/FourierSeries.html

Fourier Transform:

For this part find the following link

https://math.stackexchange.com/tags/fourier-transform/info

10420 questions
1
vote
1 answer

Question on Parseval's theorem

If $\sum_{k=-\infty}^{\infty}|a_k|^2$ is not finite, does Parseval's theorem say that the Fourier transform of $a_k$ is also not finite?
tag
  • 13
1
vote
1 answer

Violation of Parseval's theorem?

Can a function $f:G\to\mathbb{C}$ in $L^p,\ p>1, p\neq 2$ have a Fourier transform $F:\hat{G}\to\mathbb{C}$, where $\hat{G}$ is the Pontryagin dual space of $G$? I believe it can be shown that such a transform exists such that $F$ is in $L^q$, with…
f16
  • 11
1
vote
1 answer

distributional derivative of two variable function

Can any one help me to show that $ u(x,y) = \log |(x+y)/(x-y)| $ is locally integrable on $R^{2}$ ? I guess yes because it only can problem near $y= x$. Further how to find its distributional derivative $u_{xy}$.
user195218
1
vote
2 answers

Locally Compact Group with Haar Measure

Suppose $G$ is a locally compact abelian group, with Haar Measure $\mu$, then is $\mu(E)=\mu(E^{-1})$ for all subsets $E$ of $G$? I have seen that this is true for all Borel subsets of $G$, but I am in need of a proof and also an example showing why…
anonymous
1
vote
1 answer

FFT Autocorrelation

I'm particularly fond of a new smoothing thing "ASAP" under Stanford Future Data [Rong/Bailis]. I've been playing around with it for a couple days. I'm no stranger to Fourier transforms and frequency domains, but the math tends to be over my head. I…
jettero
  • 113
1
vote
1 answer

How to formulate arbitrary complex trigonometric polynomial?

How to formulate arbitrary complex trigonometric polynomial? I know that in real form it is $\displaystyle\sum_{n=1}^k a_n\cos(nx)+b_n\sin(nx)$
user2723
1
vote
1 answer

Fourier transform and sampling time

Given a signal $x(t)$ and the $X(\omega)$ obtained from $x(t)$ using a FFT with a sampling time $Ts$, I get a subset of $X(\omega)$: $Y(\omega)$ obtained from $X(\omega)$ taking it between $\omega_0$ and $\omega_1$, the question is: if I make the…
1
vote
1 answer

$f$ absolutely continuous, $\hat f(n) \downarrow 0$, $\hat f(n)$ positive and even, then $\sum \hat f_n <\infty$

Suppose $f$ is absolutely continuous and the Fourier coefficients of $f$ satisfy $$ \hat f(n)= \frac{a_n sgn(n)}{n} \ge 0 $$ where the $a_n$ are postive, even, and decreasing to zero as $|n| \to \infty$, so that the Fourier coefficients of $f$ are…
user14108
1
vote
2 answers

evaluate the Fourier transform $\int^\infty _{-\infty} \frac{sint}{t}e^{iwt}dt $

I want to evaluate $$\int^\infty _{-\infty} \frac{sin^2t}{t^2}dt $$ using Parseval's identity. For that I first have to evaluate the Fourier transform $$\int^\infty _{-\infty} \frac{sint}{t}e^{iwt}dt $$ I am stuck here. How to evaluate this…
mathemather
  • 2,959
1
vote
1 answer

Showing that the function is decreasing

$y$ is a solution to the diff-equation: $\frac{dy}{dt} = \frac{d}{dx}\frac{dy}{dx}$ for $0\le x\le\pi$ and $t\ge 0$. It also fulfills $y(0,t)=y(\pi,t)=0$ for $t\ge 0$. I want to show that $\int_{0}^{\pi} (y(x,t))^{2} dx\,\,\,is\, a\, decreasing\,…
fejz1234
  • 542
1
vote
1 answer

Stuck with proving value of series

I have the function $y(x)=e^{iax}, a\in\mathbb{R}$. Where $0\le x\le 2\pi$, and y(x) is also $2\pi$-periodic. They asked me to find the fourier coefficients of y(x), which I found out to be $\frac{e^{i2\pi a}-1}{2\pi i(a-n)}$. But I'm also asked to…
fejz1234
  • 542
1
vote
0 answers

Computing fourier coefficients

Im given that $J_n(x)$ are the fourier coefficients of $e^{ix\cdot\sin t} = \sum_{-\infty}^\infty J_n(x)e^{int}.$ I want to show that the sum $\sum_{-\infty}^\infty |J_n(x)|^2$ is not dependent on the variable $x$. I was thinking that the since the…
fejz1234
  • 542
1
vote
1 answer

variables of Fourier analysis - how to prove their relations

Fourier transform: $\hat{f}(\xi) = \int_{-\infty}^{\infty} f(t)\ e^{- 2\pi i t \xi}\,dx$ where $t$ can be time and $\xi$ can be frequency. So, the question is how do we prove that $t$ and $\xi$ can in fact be time-frequency combination?
1
vote
0 answers

If $\hat f$ the fourier transform of $f$ does $f(x)$ the fourier transform of $\hat f(-x)$?

Let $f:\mathbb R\longrightarrow \mathbb R$ a function. The Fourier transform is given by $$\hat f(\alpha )=\int_{\mathbb R}f(x)e^{-2i\pi \alpha x}dx$$ and the inversion by $$f(x)=\int_{\mathbb R}\hat f(\alpha )e^{2i\pi \alpha x}d \alpha .$$ If I set…
user330587
  • 1,624
1
vote
1 answer

Fourier transform, why this gives incorrect answer?

Let $f(x) = \begin{cases}e^{-x} & ,0
0912
  • 458